Lead-core shielding doors for 6–10 MV linear accelerators — engineered per NCRP 151 for bunkers where photon attenuation alone provides full protection.
Linear accelerators operating at 6 MV — and in most configurations up to 10 MV — stay below the practical threshold where photonuclear reactions in the machine head begin producing a significant neutron field. For these vaults, the door at the maze entrance has one job: attenuating scattered photons and head-leakage radiation to the design dose limit behind the door. That job is done with high-density material, and it is done best with lead.
Because no hydrogenous neutron-moderating layer is required, low energy LINAC doors are thinner, lighter and more economical than their high-energy counterparts — which opens up design freedom: hinged single-leaf doors, compact sliding systems, or manual operation where clinical workflow allows it.
Every MSA Projecta low energy door is built around a continuous virgin-lead core (ASTM B-29, maximum 3% thickness variation) fully encapsulated in a welded steel chassis. The lead thickness is never a catalogue value: it is calculated for your specific project from the bunker drawings, maze geometry, machine workload, use factors and the occupancy of the area behind the door, following NCRP Report No. 151 methodology.
| Parameter | Typical Configuration |
|---|---|
| Energy range | 6 MV single energy · 6/10 MV dual energy |
| Shielding core | Continuous lead sheet/brick core, steel encapsulation |
| Door types | Hinged (single/double leaf) or sliding |
| Operation | Manual, electro-mechanical or fully automatic PLC-controlled |
| Safety systems | Interlock circuit, presence detection, emergency release, battery backup |
| Design basis | NCRP 151 · IAEA Safety Reports Series No. 47 · local regulatory limits |
In a properly designed maze bunker, the door receives only multiply-scattered radiation, so the required lead thickness stays modest and the door remains light enough for smooth manual or hinged operation. In space-constrained facilities without a maze, the door itself becomes part of the secondary barrier — a direct-shielded door — and its lead content grows substantially, which usually dictates a motorized sliding design. We engineer both configurations and advise at the project design stage which layout serves your floor plan, patient throughput and budget best.
Yes. At 6 MV the photoneutron yield from the accelerator head is negligible, so the door only needs to attenuate scattered and leakage photons. A properly calculated lead core provides complete protection without any neutron-absorbing layer.
There is no universal value — the thickness comes out of the NCRP 151 calculation for your specific bunker. At the end of a well-designed maze the lead requirement is modest; in a direct-shielded (mazeless) layout it increases substantially. We provide the exact specification with the shielding report for your project.
A door specified for 6–10 MV photon shielding will generally not meet the neutron shielding requirements of a 15–18 MV machine. If a future energy upgrade is realistic for your facility, tell us at the design stage — we can dimension the door chassis and rail system so shielding layers can be added later at far lower cost than full replacement.
If your maze and corridor space allow the swing arc, a hinged door is the most economical and mechanically simplest solution. Sliding doors win where corridor space is tight, where the door is heavy, or where fully automatic operation is preferred for patient throughput.